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US5229670A - Linear motor device having vibration reduction unit - Google Patents

Linear motor device having vibration reduction unit
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US5229670A
US5229670AUS07/798,933US79893391AUS5229670AUS 5229670 AUS5229670 AUS 5229670AUS 79893391 AUS79893391 AUS 79893391AUS 5229670 AUS5229670 AUS 5229670A
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magnetic field
movable member
vibration
linear motor
driving
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Toshiaki Kagawa
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Sharp Corp
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Sharp Corp
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Abstract

An improved linear motor device is disclosed having a vibration reduction unit. The linear motor device can be applied to a copying machine. As a magnetic field forming device receives reaction force and is moved, in the opposite direction to the movement of movable members, vibration is not transmitted to a base frame. The magnetic field forming device is carried to a most suitable position for absorbing the vibration by a driving device employing a pulse motor. A velocity reduction ratio in a velocity reduction mechanism of the driving device is set to be different from a velocity reduction ratio under an ideal condition in which frictional force is neglected. As a result, the magnet field forming device can be driven by a smaller pulse motor.

Description

CROSS-REFERENCE TO RELATED APPLICATIONS
This application is related to copending U.S. Pat. application Ser. No. 07/509,806 particular interest, entitled "A LINEAR DRIVING APPARATUS", filed Apr. 17, 1990, and assigned to the same assignee of the present invention.
BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates generally to linear motor device and, more particularly, relates to an improved linear motor device having a vibration reduction unit. The present invention has particular applicability to copying machines.
2. Description of the Background Art
Linear motors have been widely used for various kinds of industrial equipment including electronic equipment requiring linear movement. While a linear motor can move a movable member to be carried in a quick and precise manner, vibration is caused by the movement. If the vibration is transmitted to another components within the equipment employing the linear motor, in some cases, a malfunction or a problem is caused to the components. Particularly, as electronic equipment such as a copying machine and optical or magnetic disc apparatus employing a linear motor encounters a serious problem caused by the vibration, various measures are taken in order to prevent or reduce the vibration.
For example, in optical or magnetic disc apparatus, a movable unit including a voice coil is mounted on a rectilinearly movable member and a magnetic field forming member including permanent magnet is fixed on a base frame. When the movable member is moved, the voice coil is driven and a thrust is caused at the movable unit. The magnetic field forming member receives reaction force corresponding to the thrust and the reaction force is transmitted to the base frame. As a result, vibration is caused in the base frame or, in some cases, the shape of the base frame is changed, which often causes malfunction in data access, i.e., data reading/writing in the optical or magnetic disc apparatus.
While the present invention is applicable to various kinds of equipment including a copying machine and optical or magnetic disc apparatus employing a linear motor, a description will be made of one example where the present invention is applied to a copying machine in the following.
FIG. 1 is a block diagram of a conventional copying machine. Referring to FIG. 1, the copying machine includes twomovable members 10a and 10b which move linearly along anoriginal document surface 64. There are provided onmovable member 10a ahalogen lamp 102 for directing light for reading out an image onto the original document and areflecting mirror 101 for reflecting the reflected light from the original document. Two reflectingmirrors 103 and 104 are provided onmovable member 10b, for reflecting light directed from reflectingmirror 101. The light reflected by reflectingmirror 104 is given to a reflectingmirror 66 through azoom lens 65. The light reflected by reflectingmirror 66 is irradiated on aphotoreceptor drum 67. It is noted that reflectingmirrors 101, 103, 104 and 66 are provided for changing the light path of the light supplied from the original document.
A developingunit 69 supplies toner tophotoreceptor drum 67 according to the light directed onphotoreceptor drum 67. Accordingly, atoner image 70 is formed onphotoreceptor drum 67 and the toner image is transferred onto arecording paper 72, which is prepared in advance, by atransfer unit 71. The transferred image is fixed onrecording paper 72 by afixing unit 73. Adischarging unit 74 eliminates electric charge left onphotoreceptor drum 67. Acleaner 75 is provided for removing the toner left onphotoreceptor drum 67. The surface ofphotoreceptor drum 67 is restored to its initial state by acharging unit 68.
FIG. 3 is a plan view of a copying machine representing the background of the present invention. The copying machine shown in FIG. 3 has been already proposed in the earlier application by the applicant of the present invention. Referring to FIG. 3, the copying machine includes abase frame 1, a magneticfield forming device 36 movable in the lateral direction, that is, the directions A and B, andmovable members 10a and 10b each capable of moving independently from each other in the lateral direction.Movable members 10a and 10b correspond tomovable members 10a and 10b shown in FIG. 1, respectively. Accordingly,movable member 10a shown in FIG. 3 includes ahalogen lamp 102 and a reflecting mirror 101 (not shown).Movable member 10b also includes reflectingmirrors 103 and 104 (not shown). It is noted that thesemovable members 10a and 10b are moved with the velocity ratio of 2:1 in order to keep constant the light path length of the light reflected from the original document.Movable members 10a and 10b move in the direction B in the return operation after moving in the direction A in the scanning operation.
Twoholders 2 are attached onbase frame 1 and arail 3 is held byholders 2.Movable member 10a moves alongrail 3 through abearing 11a.Movable member 10b also moves alongrail 3 through abearing 11b.
Movable units 20a are provided on both ends ofmovable member 10a. Similarly,movable units 20b are provided on both ends ofmovable member 10b. Magneticfield forming members 30a and 30b facingmovable units 20a and 20b are provided within a magneticfield forming device 36.Linear encoders 13a and 13b are formed onmovable members 10a and 10b, respectively. Astator scale 13c is attached onbase frame 1 through two fixedmembers 5.Linear encoders 13a and 13b detect the present positions ofmovable members 10a and 10b onstator scale 13c.
Magneticfield forming member 30a includes a platelikepermanent magnet 32a and afixed yoke 31a. Similarly, magneticfield forming member 30b includes a plate-likepermanent magnet 32b andfixed yoke 31b. Magneticfield forming members 30a and 30b are coupled to each other by connectingplates 33 and 34. Accordingly magneticfield forming device 36 is formed of magneticfield forming members 30a, 30b and connectingplates 33, 34. Twobearings 35 for supportingguide rail 3 is provided inside magneticfield forming member 30a.
FIG. 2 is a structural cross-sectional view taken along the line V--V in FIG. 3. Referring to FIG. 2, arail 4 is attached at the upper side ofbase frame 1 and aroller 12a runs onrail 4.Movable member 10a is connected toroller 12a by a connectingmember 22a. A total of tworollers 6 are provided under magneticfield forming member 30b and onbase frame 1, so that magneticfield forming device 36 can move in either direction A or B onbase frame 1.
Movable unit 20a includesmovable yokes 21a and 22a attached on both sides ofmovable member 10a and two three-phase coils 23a attached outside ofmovable yokes 21a and 22a. A three-phase brushless linear motor is made up of the two three-phase coils 23a andpermanent magnets 32a and 32b facing three-phase coils 23a and formed inside fixedyokes 31a and 31b. Hole elements (not shown) are provided at predetermined positions onmovable yokes 21a and 22a for detecting a timing for magnetization switching of three-phase coils 23a. The hole elements detect the change of magnetic fluxes ofpermanent magnets 32a, 32b. Similarly, another three-phase brushless linear motor is made up of twomovable units 20b and magneticfield forming members 30a and 30b.
Referring back to FIG. 3,struts 41a and 41b are provided outside offixed yoke 31a of magneticfield forming device 36. FIG. 4 is a structural cross-sectional view taken along the line W--W in FIG. 3.Struts 41a and 41b extend through twoholes 42a and 42b formed in the side surface of the base frame. Apulley 45 on which awire 43 having a predetermined tension is wound is provided betweenstruts 41a and 41b and outside ofbase frame 1.Pulley 45, along with a timingpulley 46, is provided inside agear box 47 attached outside ofbase frame 1.Pulley 45 and timingpulley 46 are connected to each other through atiming belt 48. Apulse motor 49 is provided outside ofgear box 47 and a rotation shaft ofpulse motor 49 is connected to timingpulley 46. As a result, magneticfield forming device 36 can be moved by drivingpulse motor 49. In other words,wire 43,pulley 45, timingpulley 46,timing belt 48 andpulse motor 49 constitute a drivingdevice 40 for driving magneticfield forming device 36.
Timingpulley 46 is rotated by drivingpulse motor 49. Astiming belt 48 transmits the rotation of timingpulley 46 topulley 45, the rotating velocity ofpulley 45 is changed with a predetermined reduction gear ratio or velocity reduction ratio. The rotation ofpulley 45 transmits its power to magneticfield forming device 36 throughwire 43 and struts 41a and 41b. Accordingly, magneticfield forming device 36 is moved in the direction A or B inbase frame 1. The detail of drivingdevice 40 in FIG. 3 is shown in FIG. 6.
FIG. 5 is a block diagram of amotor control circuit 50 and a motor driving circuit 60 for controlling and drivingpulse motor 49 shown in FIG. 3. Referring to FIG. 5, there are provided inmovable member 10a three-phase coil 23a as an armature winding, andlinear encoder 13a for detecting the position ofmovable member 10a. Similarly, three-phase coil 23b andlinear encoder 13b are provided inmovable member 10b. Each positional detection signal supplied bylinear encoders 13a and 13b includes two rectangular wave signals having a phase difference of 90° each other and a home position detection signal. The positional detection signal is supplied to a microprocessor (MPU) 51 throughwaveform shapers 51a and 51b, and the present positions and moving velocities ofmovable members 10a and 10b are obtained inmicroprocessor 51.
Microprocessor 51 includes a memory (not shown) in which the movement positional data and velocity data ofmovable members 10a and 10b are stored in advance.Microprocessor 51 compares the stored positional data with the present positional data detected and supplies a three-phase driving signal for driving the linear motors to three-phase drivers 52a and 52b based on the result of the comparison. Three-phase drivers 52a and 52b supply three-phase driving signals for driving three-phase coils 23a and 23b in response to the driving signal supplied frommicroprocessor 51.
That is,motor control circuit 50 receives the positional detection signals supplied fromlinear encoders 13a and 13b as feedback signals and controls the positions and velocities of two linear motors independently from each other.
Motor driving circuit 60 includes aninput selection switch 61, alogic circuit 62 and a four-phasecurrent driver circuit 63. A count up pulse Up and a count down pulse Dn are supplied to one input S ofswitch 61 frommotor control circuit 50. A count up pulse Upi and a count down pulse Dni in the initial state are provided to the other terminal I ofswitch 61.
When the power supply is turned on,switch 61 is connected to terminal I and magneticfield forming device 36 is moved to a position defined by the initializing signals Upi and Dni. Asswitch 61 is connected to terminal S after the initialization is completed, the count up pulse Up and the count down pulse Dn indicating the position ofmovable member 10a are supplied tologic circuit 62 throughswitch 61. A predetermined logic processing is carried out inlogic circuit 62 and an output signal therefrom is supplied to four phasecurrent driver circuit 63. Four phasecurrent driver circuit 63 supplies driving currents of four phases topulse motor 49 so that magneticfield forming device 36 is moved.
Movable members 10a and 10b are moved with the velocity ratio of 2:1 as stated above. The changes in the velocities Va and Vb ofmovable members 10a and 10b are shown in FIG. 7A. In FIG. 7A, the axis of abscissas represents the passage of time t and the axis of ordinates represents velocity V.
Asmovable members 10a and 10b are moved according to the velocity patterns shown in FIG. 7, the respective positions Xa and Xb ofmovable members 10a and 10b change as shown in FIG. 7B. In FIG. 7B, the axis of ordinates represents a distance X of movement with the direction A shown in FIG. 3 being positive.
As shown in FIGS. 7A and 7B, when the original document is scanned, the twomovable members 10a and 10b are moved according to the velocity patterns and positional patterns shown in FIGS. 7A and 7B (the data is stored in the memory within microprocessor 51). The propulsion force for movingmovable members 10a and 10b is obtained by the linear motors which have already been described. That is, as shown in FIG. 2,movable member 10a obtains the propulsion force from the two linear motors including magneticfield forming members 30a and 30b and three-phase coils 23a. Similarly,movable member 10b also receives another propulsion force. Asmovable members 10a and 10b receive the propulsion force from magneticfield forming members 30a and 30b through electromagnetic coupling, magneticfield forming members 30a and 30b also receive reaction forces from the twomovable members 10a and 10b. Though the magnitudes of the reaction forces are the same as those ofmovable members 10a and 10b, they are applied in the opposite direction. Accordingly, magneticfield forming device 36 is moved by the reaction force.
FIG. 7C indicates a distance Y of movement of magneticfield forming device 36. The positive direction of movement of magneticfield forming device 36 in FIG. 7C is opposite to that ofmovable members 10a and 10b in FIG. 7B. Asmovable members 10a and 10b move in the scanning direction A in the scanning period Ts, magneticfield forming device 36 moves in the opposite direction B in this period. Conversely, asmovable members 10a and 10b move in the direction B in the return period Tr, magneticfield forming device 36 is moved in the direction A by the reaction force. As a result, the reaction force Fr caused by the movement ofmovable members 10a and 10b is not transmitted tobase frame 1, so that the vibration caused by the movement ofmovable members 10a and 10b is not transmitted tobase frame 1.
A curved line Y1 shown in FIG. 7C is obtained assuming that there is no frictional force Fμ in the movement of magneticfield forming device 36. Actually, as frictional force Fμ (>0) is caused between magneticfield forming device 36 andbase frame 1 with the movement, magneticfield forming device 36 is moved according to the curved line Y2 in FIG. 7C. That is, as there is frictional force Fμ, which is not negligible, between magneticfield forming device 36 andbase frame 1, magneticfield forming device 36 can not be returned to its original position only by the reaction force frommovable members 10a and 10b.
Supposing that the propulsion forces ofmovable members 10a and 10b are Fa (t) and Fb (t), and frictional forces ofmovable members 10a and 10b and magneticfield forming device 36 are Fμa, Fμb and Fμm, respectively, forces Fl (t), F2 (t) and Fm (t) acting onmovable members 10a and 10b and magneticfield forming device 36 are obtained in accordance with the following equations: ##EQU1##
In this case, if Fμa+Fμb-FμM is defined as a friction load loss Fμ, the following relation holds true, so that the relation of Fμ>0 is obtained asmovable members 10a and 10b are supported by plain bearings while magneticfield forming device 36 is supported by a ball-and-roller bearing:
Fμa+Fμb>Fμm                                       (6).
The velocity reduction ratio of the velocity reduction mechanism ofpulse motor 49 shown in FIG. 6 is so adapted that the load ofpulse motor 49 is 0 under the ideal condition (Fμ=0). Supposing that x is the velocity reduction ratio of the velocity reduction mechanism and r is the radius ofwire pulley 45, the torque T generated at the rotation shaft ofpulse motor 49 is expressed by the following equation:
T=(1/x)·r·Fμ                          (7).
If Fμ=0, the electrical angle of a field winding inpulse motor 49 always coincides with the rotor rotation angle ofpulse motor 49 to whichwire 43,pulley 45 and so on are coupled, so that no rotating force is caused in the rotor ofpulse motor 49. That is,pulse motor 49 is operated under a no-load condition.
Conversely, if there is friction load loss Fμ, the electrical angle of the field winding ofpulse motor 49 does not coincide with the rotor rotation angle ofpulse motor 49, so that rotating force is generated in the rotor ofpulse motor 49 in such a direction that the difference therebetween is reduced. The rotating force is transmitted to magneticfield forming device 36 throughwire 43,pulley 45 and so on, so that magneticfield forming device 36 is controlled in the same way as in the case where Fμ=0. Accordingly, also in the case where Fμ>0, magneticfield forming device 36 is returned to the exact, initial position after the scanning operation as indicated by the curved line Y3 shown in FIG. 8A.
In this way, magneticfield forming device 36 is always moved to a desired position by the action ofpulsemotor 49 in the copying machine shown in FIG. 3. The following problems, however, are pointed out. That is, as the friction load loss Fμ becomes larger, a larger output torque is required forpulse motor 49. If the friction load loss Fμ is excessively larger than the maximum output torque of pulse motor 49 (Fμ>>0), a step-out is caused inpulse motor 49. As the driving frequency ofpulse motor 49 changes as shown in FIG. 8B, the step-out is likely to be caused particularly in the latter half period Td in the return period. If the step-out is caused inpulse motor 49, magneticfield forming device 36 is not returned to the desired initial position as indicated by the broken line Y3' in FIG. 8A. As a result, in the next scanning operation, a problem is caused such as a collision ofmovable members 10a and 10b withbearings 35 or a collision of connectingplates 33 and 34 withholders 2.
In order to prevent the step-out ofpulse motor 49, it is necessary to use, asmotor 49, a pulse motor having a larger maximum output torque. A pulse motor having a larger output torque, however, is generally large, so that the size and cost of the copying machine is inevitably increased.
SUMMARY OF THE INVENTION
An object of the present invention is to miniaturize a driving device for driving a vibration reduction unit in a linear motor device including the vibration reduction unit.
Another object of the present invention is to prevent false movement of a vibration reduction unit in a linear motor device including the vibration reduction unit without increasing the device size.
Still another object of the present invention is to miniaturize a driving device for driving a vibration reduction unit in a copying machine including the vibration reduction unit.
Yet another object of the present invention is to prevent false movement of a vibration reduction unit in a copying machine including the vibration reduction unit without increasing the device size.
In short, a linear motor device according to the present invention includes a linearly movable member which is moved linearly, an armature winding formed on the linearly movable member, a vibration reduction unit which is moved in an opposite direction to that of the movement of the linearly movable member, for reducing vibration caused by the movement of the linearly movable member, a magnetic field device formed on the vibration reduction unit and coupled to the armature winding through a magnetic field, a driving device for driving the vibration reduction unit and the magnetic field device in the opposite direction to that of the movement of the linearly movable member under an ideal condition in which frictional force is neglected, and an electromagnetic coupling reduction means for reducing electromagnetic coupling between the armature winding and the magnetic field device.
In operation, as the electromagnetic coupling reduction means reduces electromagnetic coupling between the armature winding and the magnetic field device, the output required for the driving device is reduced.
In accordance with another aspect of the present invention, a copying machine includes a light source for applying light for reading an image onto an original document, first and second reflecting units for changing the light path of a reflected light from the original document, and a transfer device responsive to the reflected light transmitted through the first and second reflecting units for transferring a read out image onto a recording medium which is prepared in advance. The first and second reflecting units are moved independently and linearly in parallel to the original document so as to keep the light path length of the reflected light at a fixed value. The copying machine further includes first and second armature windings formed on the first and second reflecting units, respectively, a vibration reduction unit which is moved in the opposite direction to that of the movement of the first and second reflecting units, for reducing vibration caused by the movement of the first and second reflecting units, a magnetic field device formed on the vibration reduction unit and coupled to the first and second armature windings through the magnetic field, a driving device for driving the vibration reduction unit and the magnetic field device in the opposite direction to that of the movement of the first and second reflecting units under an ideal condition in which frictional force is neglected, and electromagnetic coupling reduction means for reducing electromagnetic coupling between the first and second armature windings and the magnetic field device.
The foregoing and other objects, features, aspects and advantages of the present invention will become more apparent from the following detailed description of the present invention when taken in conjunction with the accompanying drawings.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a block diagram of a conventional copying machine.
FIG. 2 is a structural cross-sectional view taken along a line V--V in FIG. 3.
FIG. 3 is a plan view of a copying machine representing the background of the invention.
FIG. 4 is a structural cross-sectional view taken along the line W--W in FIG. 3.
FIG. 5 is a block diagram of a motor control circuit for controlling and driving the pulse motor shown in FIG. 3.
FIG. 6 is a structural drawing showing the structure of the driving device shown in FIG. 3.
FIG. 7A is a velocity change diagram showing changes in velocities of movement of two movable members.
FIG. 7B is a movement change diagram showing changes in movement of the two movable members.
FIG. 7C is a movement change diagram showing the change of movement of a magnetic field forming device which changes depending on whether there is a friction load loss.
FIG. 8A is a movement change diagram showing the change of movement of the magnetic field forming device in a case where a driving device is provided.
FIG. 8B is a frequency change diagram showing the change in the driving frequency of a pulse motor in the driving device.
FIG. 9A is a movement change diagram showing the change of movement of a magnetic field forming device in accordance with one embodiment of the present invention.
FIG. 9B is a frequency change diagram showing the change in the driving frequency of a pulse motor in accordance with one embodiment of the present invention.
FIG. 9C is a torque change diagram showing the change in the output torque of the pulse motor in accordance with one embodiment of the present invention.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
In a preferred embodiment, the velocity reduction ratio of a velocity reduction mechanism in the driving device shown in FIG. 6 is changed as described below in detail. That is, the velocity reduction ratio x under the ideal condition (Fμ=0) is changed and a new velocity reduction ratio x' is set. The value of the new velocity reduction ratio x' is set to be slightly larger or smaller than the velocity reduction ratio x under the ideal condition. As a result, the movement of magneticfield forming device 36 is changed with the new velocity reduction ratio x' as indicated by the broken line Y5 in FIG. 9A. The solid line Y4 in FIG. 9A represents for reference the change in the movement of magneticfield forming device 36 in the case where the ideal velocity reduction ratio x is set. In the example shown in FIG. 9A, the new velocity reduction ratio x' is set to be slightly larger than the ideal velocity reduction ratio x. As seen from FIG. 9A, the distance Y5 of movement of magneticfield forming device 36 is slightly reduced with the new velocity reduction ratio x' compared with the distance Y4 of movement with the ideal velocity reduction ratio x.
Assuming that the mass of magneticfield forming device 36 is M, and the acceleration of magneticfield forming device 36 with the velocity reduction ratio x is α (t), the acceleration α' (t) with the velocity reduction ratio x' is obtained according to the following equation:
α'(t)=(x/x')·α (t)                    (8).
Accordingly, force exerted on magneticfield forming device 36 with the new velocity reduction ratio x' is excessively changed by ΔF represented by the following equation, compared with the value with the velocity reduction ratio x: ##EQU2##
As the force ΔF acts in the opposite direction to that of the friction load loss Fμ in the latter half period Td in the return period (see FIG. 9B), the torque T' applied on the rotation shaft ofpulse motor 49 is expressed by the following equation:
T'=(1/x')·r·(Fμ-ΔF)             (10).
As a result, the load of the rotation shaft ofpulse motor 49 can be reduced as indicated by the broken line T' in FIG. 9C. This means that the step-out is prevented even if a pulse motor with a smaller output torque is used aspulse motor 49 of drivingdevice 40. Accordingly, magneticfield forming device 36 can be driven by a smaller pulse motor and returned to the exact, initial position.
A detailed description will be made below of a range in which the new velocity reduction ratio x' is set. At first, a description will be made of the ideal condition, that is, an ideal velocity reduction ratio x in the case where there is no friction load loss Fμ. Suppose that the velocities ofmovable members 10a and 10b and magneticfield forming device 36 are Va, Vb and Vm, respectively. Also, suppose that the respective masses ofmovable members 10a and 10b and magneticfield forming device 36 are Ma, Mb and Mm. Vm is expressed by the following equation under the ideal condition (Fμ=0): ##EQU3##
The velocity reduction ratio x is expressed by the following equation:
x=|Va/Vm|=Mm/(Am+Mb/2)                   (12).
In addition, the following variables are given for drivingdevice 40 shown in FIG. 6:
θ;a rotation angle (radian) ofpulse motor 49 with respect to the distance of movement ofmovable member 10a;
Z1; the number of teeth of timingpulley 46;
Z2; the number of teeth of timingpulley 45a;
Dp; a diameter ofwire pulley 45b; and
Dw; a diameter ofwire 43.
Accordingly, the velocity reduction ratio x is expressed by the following equation:
x={θ·(Z1/Z2)·(Dp+Dw)/2}.sup.-1     (13).
If Ma=1.8 (kg), Mb=2.4 (kg), and Mm=15 (kg) are given as actual data, the velocity reduction ratio x under the ideal condition is obtained according to the expression (12) as indicated by the following equation:
x=15/(1.8+2.4/2)=5                                         (14).
Therefore, in the copying machine representing the background of the invention, the velocity reduction mechanism shown in FIG. 6 was designed to obtain x=5 with Fμ=0 as follows: θ=τ/90 (rad / mm), Z1=20, Z2=60, Dp=33.4 (mm), Dw=1.0 (mm).
In a preferred embodiment, the variables included in the expression (13) can be changed in order to set a new velocity reduction ratio x'. For example, if the number Z1 of teeth of timingpulley 46 is set at 18, x'=5.56 is obtained. In another case, if the number Z2 of teeth of timingpulley 45a is set at 67, x'=5.58 is obtained. In still another case, if the diameter Dp ofwire pulley 45b is set at 30 (mm), x'=5.54 is obtained. The new velocity reduction ratio x' can be changed by not only modifying just one variable as stated above but by modifying two or more variables included in the expression (13).
A description will now be made of a permissible range in which a new velocity reduction ratio x' is set. In an experiment, it was observed whether there was step-out of the pulse motor and the magnitude of vibration transmitted tobase frame 1 was measured according to several kinds of velocity reduction ratios x' obtained by changing the number Z1 of teeth of timingpulley 46 to several values. The result of the measurement is shown in the following table 1.
              TABLE 1                                                     ______________________________________                                    Number Z1  Velocity              Vibration of                             of teeth of                                                                          reduction Step-out ofBase frame 1timing pulley 46                                                                     ratio x'  pulse motor 49                                                                        (mm)                                     ______________________________________                                    16         6.25      not observed                                                                          0.16                                     17         5.88      not observed                                                                          0.13                                     18         5.56      not observed                                                                          0.11                                     19         5.26      observed     0.098                                   20         5         observed     0.092                                   ______________________________________
A seen from the result of the experiment shown in Table 1, if the value of the velocity reduction ratio x' is set larger, the step-out ofpulse motor 49 is prevented and vibration ofbase frame 1 increased. That is, setting a larger velocity reduction ratio x' lowers the capability of absorbing the reaction force by magneticfield forming device 36 and increases the vibration transmitted tobase frame 1. In view of the result of the experiment above, the velocity reduction ratio x' is set at such a value that a step-out is not caused inpulse motor 49 within a range where the vibration ofbase frame 1 is permissible, for example, x'=5.56 (Z1=18). The vibration (displacement) ofbase frame 1 is 0.11 (mm) with x'=5.56, which is sufficiently small compared with the vibration (=5.56 mm) of base frame in a case where there is no mechanism provided for reducing the reaction force. In other words, the reduction of the function of absorbing the reaction force with x'=5.56 is not actually a serious problem.
As stated above, vibration caused bymovable members 10a and 10b can be reduced or absorbed without using a large pulse motor by changing the velocity reduction ratio of the velocity reduction mechanism in drivingdevice 40 shown in FIG. 6 to the value x' slightly larger or smaller than the value x under the ideal condition (Fμ=0). In other words, drivingdevice 40 for driving a vibration absorbing unit, i.e., magneticfield forming device 36 can be miniaturized without causing false movement of a vibration reduction unit.
Although the present invention has been described and illustrated in detail, it is clearly understood that the same is by way of illustration and example only and is no to be taken by way of limitation, the spirit and scope of the present invention being limited only by the terms of the appended claims.

Claims (7)

What is claimed is:
1. A linear motor device, comprising:
a linearly movable member moved linearly;
armature winding means formed on said linearly movable member;
vibration reduction means which is moved in the opposite direction to the movement of said linearly movable member, for reducing vibration caused by the movement of said linearly movable member;
magnetic field means formed on said vibration reduction means and coupled to said armature winding means through an electromagnetic field, the vibration caused by the movement of said linearly movable member being transmitted to said vibration reduction means through said armature winding means and the magnetic field means;
driving means for driving said vibration reduction means and the magnetic field means in the opposite direction to the movement of said linearly movable member under an ideal condition in which frictional force is neglected; and
electromagnetic coupling reduction means for reducing electromagnetic coupling between said armature winding means and the magnetic field means.
2. The linear motor device according to claim 1, wherein said vibration reduction means includes reaction force absorbing means for absorbing reaction force from said movable member through the electromagnetic coupling between said armature winding means and the magnetic field means to reduce said vibration caused by the movement of said movable member.
3. The linear motor device according to claim 1, wherein said driving means includes:
rotation power generating means for generating rotation power for moving said vibration reduction means and the magnetic field means; and
reduction gear means for changing the velocity of the rotation power generated from said rotation power generating means with a predetermined velocity reduction ratio under said ideal condition, and
wherein said vibration reduction means and the magnetic field means is driven by the rotation power output from said reduction gear means.
4. The linear motor device according to claim 3, wherein said driving means further includes:
positional detection means for detecting a position of said linearly movable member; and
rotation control means responsive to a detected position of said linearly movable member for controlling an output from said rotation power generating means.
5. The linear motor device according to claim 3, wherein said electromagnetic coupling reduction means includes velocity reduction ratio changing means for changing said predetermined velocity reduction ratio of said velocity reduction gear means by a predetermined value to reduce the electromagnetic coupling between said armature winding means and the magnetic field means.
6. The linear motor device according to claim 5, wherein said predetermined value is determined according to a relation between a permissible amount of vibration in said linear motor device and the maximum rotation power which can be supplied from said rotation power generating means.
7. The linear motor device according to claim 4, wherein
said rotation power generating means includes a pulse motor for generating rotation power,
said rotation control means includes a microprocessor responsive to a positional detection signal supplied from said positional detection means for generating a driving pulse for driving said pulse motor, and
said pulse motor is driven by the driving pulse generated from said microprocessor.
US07/798,9331990-11-301991-11-27Linear motor device having vibration reduction unitExpired - LifetimeUS5229670A (en)

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JP2338736AJP2752248B2 (en)1990-11-301990-11-30 Linear motor device
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US5796186A (en)*1995-03-311998-08-18Minolta Co., Ltd.Linear motor
US5801462A (en)*1995-03-311998-09-01Minolta Co., Ltd.Linear motor and image reading apparatus
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US5955798A (en)*1995-03-311999-09-21Minolta Co., Ltd.Linear motor
US6012346A (en)*1998-09-182000-01-11New Hampshire Ball Bearing, Inc.Low vibration motion translation system
US6028376A (en)*1997-04-222000-02-22Canon Kabushiki KaishaPositioning apparatus and exposure apparatus using the same
US6239517B1 (en)*1999-02-192001-05-29Hitachi Koki Co., Ltd.Linear shuttle motor assembly and a controller therefor
US6246204B1 (en)1994-06-272001-06-12Nikon CorporationElectromagnetic alignment and scanning apparatus
US6391503B2 (en)1997-09-192002-05-21Nikon CorporationScanning exposure methods
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US20060076839A1 (en)*2004-10-072006-04-13Yoichi KawaiLinear motor
US9906092B2 (en)2015-06-262018-02-27Siemens Industry, Inc.Electrodynamic machines, and method for reducing vibration of an electrodynamic machine

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US6255795B1 (en)1994-06-272001-07-03Nikon CorporationElectromagnetic alignment and scanning apparatus
US20030184253A1 (en)*1994-06-272003-10-02Nikon CorporationElectromagnetic alignment and scanning apparatus
US6844695B2 (en)1994-06-272005-01-18Nikon CorporationElectromagnetic alignment and scanning apparatus
US6844696B2 (en)1994-06-272005-01-18Nikon CorporationElectromagnetic alignment and scanning apparatus
US6969966B2 (en)1994-06-272005-11-29Nikon CorporationElectromagnetic alignment and scanning apparatus
US7573225B2 (en)1994-06-272009-08-11Nikon CorporationElectromagnetic alignment and scanning apparatus
US20050280390A1 (en)*1994-06-272005-12-22Nikon CorporationElectromagnetic alignment and scanning apparatus
US7012398B2 (en)1994-06-272006-03-14Nikon CorporationElectromagnetic alignment and scanning apparatus
US6246204B1 (en)1994-06-272001-06-12Nikon CorporationElectromagnetic alignment and scanning apparatus
US6323935B1 (en)1994-06-272001-11-27Nikon CorporationElectromagnetic alignment and scanning apparatus
US6693402B2 (en)1994-06-272004-02-17Nikon CorporationElectromagnetic alignment and scanning apparatus
US6255796B1 (en)1994-06-272001-07-03Nikon CorporationElectromagnetic alignment and scanning apparatus
US6252370B1 (en)1994-06-272001-06-26Nikon CorporationElectromagnetic alignment and scanning apparatus
US6329780B1 (en)1994-06-272001-12-11Nikon CorporationElectromagnetic alignment and scanning apparatus
US20050083006A1 (en)*1994-06-272005-04-21Nikon CorporationElectromagnetic alignment and scanning apparatus
US20030184254A1 (en)*1994-06-272003-10-02Nikon CorporationElectromagnetic alignment and scanning apparatus
US5686803A (en)*1994-10-281997-11-11Seiko Epson CorporationControl apparatus for a pulse motor
US5796186A (en)*1995-03-311998-08-18Minolta Co., Ltd.Linear motor
US5955798A (en)*1995-03-311999-09-21Minolta Co., Ltd.Linear motor
US5909066A (en)*1995-03-311999-06-01Minolta Co., Ltd.Linear motor apparatus employing linear motor as drive source
US5801462A (en)*1995-03-311998-09-01Minolta Co., Ltd.Linear motor and image reading apparatus
US6028376A (en)*1997-04-222000-02-22Canon Kabushiki KaishaPositioning apparatus and exposure apparatus using the same
US6391503B2 (en)1997-09-192002-05-21Nikon CorporationScanning exposure methods
US6012346A (en)*1998-09-182000-01-11New Hampshire Ball Bearing, Inc.Low vibration motion translation system
US6239517B1 (en)*1999-02-192001-05-29Hitachi Koki Co., Ltd.Linear shuttle motor assembly and a controller therefor
US6924882B2 (en)1999-12-212005-08-02Asml Netherlands B.V.Balanced positioning system for use in lithographic apparatus
US20040041994A1 (en)*1999-12-212004-03-04Asml Netherlands B.V.Balanced positioning system for use in lithographic apparatus
US20040119436A1 (en)*2002-12-232004-06-24Michael BinnardMethod and apparatus for reducing countermass stroke with initial velocity
US20060076839A1 (en)*2004-10-072006-04-13Yoichi KawaiLinear motor
US7154198B2 (en)*2004-10-072006-12-26Okuma CorporationLinear motor
US9906092B2 (en)2015-06-262018-02-27Siemens Industry, Inc.Electrodynamic machines, and method for reducing vibration of an electrodynamic machine

Also Published As

Publication numberPublication date
JP2752248B2 (en)1998-05-18
JPH04208095A (en)1992-07-29
DE69126768D1 (en)1997-08-14
DE69126768T2 (en)1998-02-05
EP0488805A2 (en)1992-06-03
EP0488805B1 (en)1997-07-09
EP0488805A3 (en)1994-02-02

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